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True Coincidence Summing Correction in Gamma Spectroscopy

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Germanium is the most commonly used detector material for its higher atomic<br />

number (as compared to Silicon) which makes it practicable for detection of higher<br />

energy gamma radiation. Over recent years, the technology for the manufacture of<br />

high purity germanium with a suitable degree of crystal perfection is achieved. When<br />

an n+ layer is created on a face of a high-purity p-type germanium slab (Figure-1.2)<br />

and a reverse bias is applied to the detector, a depletion layer throughout the p-type<br />

material is formed. Such a detector is called hyper-pure or simply high-purity<br />

germanium detector abbreviated as HPGe.<br />

Figure 1.2 The basic construction of germanium detector. [1]<br />

HPGe detectors are available <strong>in</strong> a number of different configurations to suit particular<br />

situations. Figure-1.3 shows the simple standard forms together with an <strong>in</strong>dication the<br />

energy range over which they might be used.<br />

Figure 1.3 Configuration of detector generally available together with the used energy range [3]<br />

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